REVIEW 43 references
High-dimensional quantum teleportation under noisy environments
Not yet reviewed by Pith; the record is open.
This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.
SPECIMEN: schema-true, not a live event
T0 review · schema-true
One-sentence machine reading of the paper's core claim.
pith:XXXXXXXX · record.json · timestamp
abstract
We study the protocol of qudit teleportation using quantum systems subjected to several kinds of noise for arbitrary dimensionality $d$. We consider four classes of noise: dit-flip, $d$-phase-flip, dit-phase-flip and depolarizing, each of them corresponding to a family of Weyl operators, introduced via Kraus formalism. We derive a general expression for the average fidelity of teleportation in arbitrary dimension $d$ for any combination of noise on the involved qudits. Under a different approach we derive the average fidelity of teleportation for a more general scenario involving the $d$-dimensional generalization of amplitude damping noise as well. We show that all possible scenarios may be classified in four different behaviours and discuss the cases in which it is possible to improve the fidelity by increasing the associated noise fractions. All our results are in agreement with previous analysis by Fortes and Rigolin for the case of qubits (Phys. Rev. A, 92 012338, 2015).
Reference graph
Works this paper leans on
-
[1]
Weyl-like noises The noise coefficient associated to the input qudit ajk may be expressed as a superposition of the contributions of each region in figure 3: a0, noiseless region (green);af, flip region (blue);ap, phase flip region (yellow) andac for the region of combination of flip and phase-flip (red). In this way, the squared noise coefficient reads a2 jk =a2 ...
-
[2]
Kraus operators in the standard computational basis Let us calculate the fidelity of teleportation. Substituting Eq. 10 in Eq. 3, we have F = ∑ jkmnµν n1n2p1p2 k1k2k3 αmα∗ nαn1α∗ p1βjµβ∗ kµγn2γ∗ p2ωµ(n−m) d a(k1) k,n1 b(k2) k⊕ν,n2 c(k3) n⊕ν,n2a(k1)∗ j,p1 b(k2)∗ j⊕ν,p2c(k3)∗ m⊕ν,p2. Analogously to the previous treatment, using the results of Appendix B and ...
- [3]
-
[4]
C. H. Bennett, G. Brassard, C. Cr´ epeau, R. Jozsa, A. Peres, and W. K. Wootters, Phys. Rev. Lett. 70, 1895 (1993)
1993
-
[5]
S. Pirandola, J. Eisert, C. Weedbrook, A. Furusawa, and S. L. Braunstein, Nature photonics 9, 641 (2015)
work page 2015
- [6]
-
[7]
And iv) the corresponding to any kind of noise in the input and Amplitude damping in the channel, depicted in Figure 8. Furthermore it was possible to note that it is possible to partially correct errors by a basis change, for a very specific case ( P, ∅, ∅). It is left as an open question whether considering special scenarios in which the nature of the in...
-
[8]
B. G. Taketani, F. de Melo, and R. L. de Matos Filho, Phys. Rev. A 85, 020301 (2012)
work page 2012
Show all 43 references
-
[9]
S. Oh, S. Lee, and H.-w. Lee, Physical Review A 66, 022316 (2002)
2002
-
[10]
L. T. Knoll, C. T. Schmiegelow, and M. A. Larotonda, Phys. Rev. A 90, 042332 (2014)
2014
-
[11]
X. Hu, Y. Gu, Q. Gong, and G. Guo, Phys. Rev. A 81, 054302 (2010)
2010
-
[12]
M. M. Cunha, E. A. Fonseca, M. Moreno, and F. Parisio, Quantum Information Processing 16, 254 (2017)
2017
-
[13]
M. G. M. Moreno, A. Fonseca, and M. M. Cunha, Quantum Information Processing 17, 191 (2018), arXiv:arXiv:1805.06517v1
2018 arXiv
-
[14]
N. J. Cerf, M. Bourennane, A. Karlsson, and N. Gisin, Phys. Rev. Lett. 88, 127902 (2002)
2002
-
[15]
T. Durt, D. Kaszlikowski, J.-L. Chen, and L. C. Kwek, Phys. Rev. A 69, 032313 (2004)
2004
-
[16]
V´ ertesi, S
T. V´ ertesi, S. Pironio, and N. Brunner, Phys. Rev. Lett. 104, 060401 (2010)
2010
-
[17]
N. T. Islam, C. C. W. Lim, C. Cahall, J. Kim, and D. J. Gauthier, Science advances 3, e1701491 (2017)
2017
-
[18]
Skrzypczyk and D
P. Skrzypczyk and D. Cavalcanti, Physical Review Let- ters 120, 260401 (2018), arXiv:1803.05199
2018 arXiv
-
[19]
X.-M. Hu, C. Zhang, B.-H. Liu, Y.-F. Huang, C.-F. Li, and G.-C. Guo, arXiv preprint arXiv:1904.12249 (2019)
2019 arXiv
-
[20]
Luo, H.-S
Y.-H. Luo, H.-S. Zhong, M. Erhard, X.-L. Wang, L.- C. Peng, M. Krenn, X. Jiang, L. Li, N.-L. Liu, C.-Y. Lu, A. Zeilinger, and J.-W. Pan, Phys. Rev. Lett. 123, 070505 (2019)
2019
-
[21]
M. Kues, C. Reimer, P. Roztocki, L. R. Cort´ es, S. Sciara, B. Wetzel, Y. Zhang, A. Cino, S. T. Chu, B. E. Little, et al., Nature 546, 622 (2017)
2017
-
[22]
R. A. Bertlmann and P. Krammer, Journal of Physics A: Mathematical and Theoretical 41, 235303 (2008)
2008
-
[23]
Horodecki, P
M. Horodecki, P. Horodecki, and R. Horodecki, Physical Review A - Atomic, Molecular, and Optical Physics 60, 1888 (1999), arXiv:9807091 [quant-ph]
1999
-
[24]
Weinar, W
R. Weinar, W. Laskowski, and M. Pawowski, Journal of Physics A: Mathematical and Theoretical 46, 435301 (2013)
2013
-
[25]
Note that this parametrization does not cover uniformly the space of pure states for two-qudits
We produced random states uniformly distributed in the basis {|00⟩,|11⟩,···| d− 1,d− 1⟩}. Note that this parametrization does not cover uniformly the space of pure states for two-qudits. Nevertheless for our purposes it is enough
-
[26]
Cavalcanti, P
D. Cavalcanti, P. Skrzypczyk, and I. ˇSupi´ c, Phys. Rev. Lett. 119, 110501 (2017)
2017
-
[27]
Carvacho, F
G. Carvacho, F. Andreoli, L. Santodonato, M. Ben- tivegna, V. D’Ambrosio, P. Skrzypczyk, I.ˇSupi´ c, D. Cav- alcanti, and F. Sciarrino, Phys. Rev. Lett. 121, 140501 (2018)
2018
-
[28]
ˇSupi´ c, P
I. ˇSupi´ c, P. Skrzypczyk, and D. Cavalcanti, Physical Review A 99, 032334 (2019), arXiv:1804.10612
2019 arXiv
-
[29]
Horodecki, P
M. Horodecki, P. Horodecki, and R. Horodecki, Physical Review Letters 80, 5239 (1998)
1998
-
[30]
M. A. Nielsen and I. L. Chuang, Quantum computation and quantum information (Cambridge university press, 2010)
2010
-
[31]
Ramzan, Quantum Information Processing 12, 577 (2013)
M. Ramzan, Quantum Information Processing 12, 577 (2013)
2013
-
[32]
Chrusci´ nski and F
D. Chrusci´ nski and F. A. Wudarski, Physical Review A - Atomic, Molecular, and Optical Physics 91, 012104 (2015), arXiv:1408.1792
2015 arXiv
-
[33]
Imany, J
P. Imany, J. A. Jaramillo-Villegas, M. S. Alshaykh, J. M. Lukens, O. D. Odele, A. J. Moore, D. E. Leaird, M. Qi, and A. M. Weiner, npj Quantum Information 5, 59 (2019)
2019
-
[34]
Gokhale, J
P. Gokhale, J. M. Baker, C. Duckering, N. C. Brown, K. R. Brown, and F. T. Chong, in Proceedings of the 46th International Symposium on Computer Architecture - ISCA ’19 (ACM Press, New York, New York, USA,
-
[35]
Here we refer to a protected qudit as one whose probabil- ity of being affected by any kind of noise is negligible in comparison with that corresponding to other components in the system
-
[36]
Miller, T
D. Miller, T. Holz, H. Kampermann, and D. Bruß, Phys- ical Review A 98, 052316 (2018), arXiv:1807.06030
2018 arXiv
-
[37]
Daniel Gottesman, Chaos, Solitons & Fractals 10, 1749 (1999)
1999
-
[38]
Dutta, J
A. Dutta, J. Ryu, W. Laskowski, and M. ukowski, Physics Letters A 380, 2191 (2016)
2016
-
[39]
˙Zyczkowski and H.-J
K. ˙Zyczkowski and H.-J. Sommers, Journal of Physics A: Mathematical and General 34, 7111 (2001)
2001
-
[40]
E. M. Laine, H. P. Breuer, and J. Piilo, Scientific Reports 4, 4620 (2014)
2014
-
[41]
C. M. Caves, Measures and volumes for spheres, the prob- ability simplex, projective Hilbert space, and density op- erators, Tech. Rep. (University of New Mexico, 2001)
2001
-
[42]
Bengtsson and K
I. Bengtsson and K. Zyczkowski, Geometry of quantum states: an introduction to quantum entanglement (Cam- bridge University Press, 2007)
2007
- [2019]
Discussion (0). Continue with ORCID to comment.